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Chemical and Physical Characterization of Poly(p-phenylene-2,6-benzobisoxazole)
Fibers Used in Body Armor:Temperature and Humidity Aging
NISTIR 7373
2
NISTIR 7373
April 2006
U.S. DEPARTMENT OF COMMERCECarlos M. Gutierrez, Secretary
TECHNOLOGY ADMINISTRATIONRobert C. Cresanti, Under Secretary of Commerce for Technology
NATIONAL INSTITUTE OF STANDARDS AND TECHNOLOGYWilliam Jeffrey, Director
Chemical and Physical Characterization of Poly(p-phenylene-2,6-benzobisoxazole)
Fibers Used in Body Armor:Temperature and Humidity Aging
Joannie Chin, Eric Byrd, Cyril Clerici, Mounira Oudina and Lipiin Sung
Polymeric Materials GroupMaterials and Construction Research Division
Building and Fire Research Laboratory
Amanda Forster and Kirk RiceOffice of Law Enforcement Standards
Electronics and Electrical Engineering Laboratory
Sponsored by:National Institute of JusticeOffice of Justice Programs
3
ABSTRACT
In recent years, poly(p-phenylene-2,6-benzobisoxazole) (PBO) fibers have
become prominent in high strength applications such as body armor, ropes and cables,
and recreational equipment. The objectives of this study were to expose woven PBO
body armor panels to elevated temperature and moisture, and to analyze the chemical,
morphological and mechanical changes in PBO yarns extracted from the panels. A 30 %
decrease in yarn tensile strength, which was correlated to changes in the infrared peak
absorbance of key functional groups in the PBO structure, was observed during the 26
week elevated temperature/elevated moisture aging period. Substantial changes in
chemical structure were observed via infrared spectroscopy, as well as changes in
polymer morphology using microscopy and neutron scattering. When the panels were
removed to an ultra-dry environment for storage for 47 weeks, no further decreases in
tensile strength degradation were observed. In a follow-on study, fibers were sealed in
argon-filled glass tubes and exposed to elevated temperature; less than a 4 % decrease in
tensile strength was observed after 30 weeks.
Key Words: body armor, poly(p-phenylene-2,6-benzobisoxazole) (PBO), attenuated
total reflectance (ATR), infrared (IR) spectroscopy, fiber, yarn, moisture sorption, tensile
strength, hydrolysis, laser scanning confocal microscopy, atomic force microscopy, small
angle neutron scattering
4
Introduction and Objectives
In recent years, high performance fibers based on poly(p-phenylene-2,6-
benzobisoxazole) (PBO) have become prominent in high strength applications such as
body armor, ropes and cables, and recreational equipment. Problems with the
performance and durability of PBO-based body armor became apparent to the law
enforcement community in the summer of 2003, when ballistic penetration of PBO-based
body armor occurred in two separate incidents.
The first incident involved the shooting of a police officer near Pittsburgh, PA
(hereinafter referred to as the “officer”) in June 2003. The bullet pierced the officer’s
PBO-based body armor, which had been manufactured less than 8 months earlier.
Mechanical testing of the yarns taken from the officer’s vest indicated a 30 % decrease in
tensile strength relative to yarns taken from new, unworn PBO-based vests of the same
model. Subsequently, another incident involving the ballistic penetration of PBO-based
body armor occurred that same year, but the evidentiary circumstances surrounding these
incidents are more complicated and, as such, are not be discussed here.
These events prompted the Department of Justice (DOJ) and then-U.S. Attorney
General John Ashcroft to announce a Body Armor Safety Initiative on November 18,
2003 [1], which tasked the National Institute of Justice (NIJ), the research, development,
and evaluation arm of DOJ, to address technical issues associated with PBO-based body
armor. In response to this initiative, NIST’s Office of Law Enforcement Standards
(OLES) and research groups within the NIST laboratories undertook a parallel, multi-
phase effort to characterize chemical and physical degradation of PBO fiber and to
correlate the observed degradation to body armor durability.
5
In previous work performed at NIST, a comparative analysis study was carried on the
officer’s vest and new, unused vests of the same make and model. The primary findings
in this work were that yarns from the officer’s vest had tensile strengths approximately
30 % lower than yarns from new vests of the same make and model, and that a
breakdown in the molecular structure of the PBO chains was revealed by infrared
analysis of the vest yarns [2].
Data from the manufacturer and the published literature have revealed the
moisture vulnerability of PBO fibers [3,4]. In an attempt to quantify this vulnerability,
and to determine if correlations existed between moisture exposure, tensile strength
degradation and ballistic failure, an experimental study was designed in which newly-
manufactured body armor constructed from PBO were exposed to elevated temperature
and relative humidity in an environmental chamber. When yarn tensile strengths had
decreased by 30 % relative to the initial tensile strength, the exposure was terminated and
ballistic testing was carried out on the exposed vest panels. The ballistic testing of the
aged vests will be documented in a separate report.
The primary goals of the work described in this report were to:
Monitor tensile strength degradation in PBO yarns extracted from body armor exposed to elevated temperature and relative humidity as a function of exposure time.
Monitor chemical and physical changes in PBO yarns extracted from body armor
exposed to elevated temperature and relative humidity as a function of exposure time.
Determine if any correlations exist between chemical hydrolysis and tensile
strength degradation in PBO yarns
6
Future phases of this research program will address degradation mechanisms, accelerated
aging and prediction of ballistic fiber service life.
Experimental Procedures*
Materials—Commercial, non-deployed body armor manufactured for this study
consisted of a ballistic panel constructed from 20 layers of woven PBO fabric stacked and
diagonally stitched together, inserted in a water vapor-permeable fabric liner, and placed
in a cotton fabric carrier. For testing and analyses, PBO yarns were extracted from the
exposed vest panels at predetermined inspection times.
Environmental Exposure— 24 ballistic panels enclosed in liners and carriers
(shown in Figure 1) were aged in a Cincinnati Sub-Zero Z32 environmental chamber at
50 oC and 60 % relative humidity (RH) for 84 d, and then 60 oC and 37 % RH for an
additional 73 d. The increase in temperature to 60 oC and decrease in relative humidity to
37 % were intended to accelerate the kinetics of fiber degradation by increasing the
temperature while maintaining the same absolute water content in the environment.
Following the completion of the environmental chamber aging, 18 panels were removed
for ballistic testing, while the remainder was stored in the chamber at 25 oC and 5 % RH
for an additional 332 d.
To more accurately monitor temperature and relative humidity in the large
chamber area, a number of temperature and RH sensors were distributed throughout the
interior of the chamber as well as in the interior of the vest panels. These temperature
* Certain commercial equipment, instruments or materials are identified in this paper in order to specify the experimental procedure adequately. Such identification is not intended to imply recommendation or endorsement by the National Institute of Standards and Technology, nor is it intended to imply that the materials or equipment identified are necessarily the best available for this purpose.
7
and RH sensor data were logged and stored via a data acquisition system and a desktop
computer.
Yarn Extraction Procedure— At each inspection time, 15 horizontally oriented
yarns were extracted from layers 1, 5, 15, 19 in two different ballistic panels (labeled 089
and 055, respectively), with two layers of each panel sampled every 2 weeks. Seams
were cut from the bottom 5 cm to 6 cm of the ballistic panel to free the layers. As shown
in Figure 2, individual yarns were loosened and extracted one by one from the lower half
of the layer using a small hook, and taped down on cleaned aluminum foil-wrapped
cardboard holders. Each yarn was labeled with panel number, layer number and yarn
number. Nitrile gloves were worn throughout the entire procedure to prevent
contamination of the yarns. From the 15 yarns extracted, three were reserved for Fourier
transform infrared (FTIR) spectroscopy analysis, while the remaining yarns were used for
tensile testing.
Moisture Sorption Analysis—Moisture absorbed by the yarn specimens during the
temperature/humidity exposure period was measured using a Hiden IGAsorp Moisture
Sorption Analyzer. The IGAsorp software monitors the temporal changes in the mass of
a specimen subjected to prescribed temperature and relative humidity conditions, and
calculates equilibrium parameters via curve fitting. Specimens for sorption analysis were
prepared by disassembling between 5 mg to 7 mg of yarn into individual filaments to
prevent capillarity effects from dominating the sorption process. Prior to beginning a
sorption experiment, specimens were dried in the moisture sorption analyzer at ≈ 0 % RH
and the prescribed temperature at which the sorption experiment would be carried out.
Moisture uptake was measured at 50 oC and 60 % RH as well as at 60 oC and 37 % RH.
8
The water sorption isotherm was generated using the isothermal mapper mode at 40 oC
within a range of 0 % RH to 95 % RH. Results are the average of two specimens. The
standard uncertainty of these measurements is typically 0.02 mass %.
Tensile Testing of Yarns and Fibers—Tensile testing of yarns was carried out in
accordance with ASTM D2256-02, “Standard Test Method for Tensile Properties of Yarn
by the Single-Strand Method”, using an Instron Model 4482 screw-driven universal test
frame equipped with a 91 kg load cell, and pneumatic yarn and chord grips (Instron
model 2714-006). Strain measurements were taken with an Instron non-contacting Type
3 video extensometer in conjunction with black foam markers placed approximately 2.5
cm apart in the gage section of the yarn. Grip separation was 7.9 cm and cross-head
speed was 2.3 cm/min. In this study, yarns were nominally 38.1 cm long, and given 60
twists on a custom-designed yarn twisting device. The standard uncertainty of measured
tensile strengths, percent strain to break, modulus, and break energy are typically ± 3 %,
± 3 %, ± 3 %, and ± 4 %, respectively.
Tensile tests were also carried out on individual single fibers utilizing a TA
Instruments RSA III, a dynamic mechanical thermal analyzer (DMTA) equipped with
transient testing capability. Specimen gage length was 25 mm and specimen extension
rate was 0.001 mm/s. A minimum of ten fibers were analyzed from one extracted yarn
per sampling interval. Standard uncertainty of tensile strengths measured using this
method is typically ± 9 %.
Fourier Transform Infrared (FTIR) Spectroscopy—Infrared analysis was carried
out using a Nicolet Nexus FTIR equipped with a mercury-cadmium-telluride (MCT)
detector and a SensIR Durascope attenuated total reflectance (ATR) accessory. Dry air
9
was used as the purge gas. Consistent pressure on the yarns was applied using the force
monitor on the Durascope. FTIR spectra were recorded at a resolution of 4 cm-1 between
4000 cm-1 and 700 cm-1 and averaged over 128 scans. Three different locations on each
yarn were analyzed. Spectral analysis, including spectral subtraction, was carried out
using a custom software program developed in the Polymeric Materials Group at NIST
[5]. All spectra were baseline corrected and normalized using the aromatic C-H
deformation peak at 848 cm-1. Standard uncertainties associated with this measurement
are typically ± 1 cm-1 in wavenumber and ± 1% in peak intensity.
Small Angle Neutron Scattering—Small angle neutron scattering (SANS)
measurements were performed at the NIST Center for Neutron Research using the 30 m
SANS instrument. Samples of virgin spool yarn, unaged vest yarn, and vest yarn aged
for 157 d in the environmental exposure study were soaked in 99 % pure deuterated water
(D2O) in a glass vial for one week, and then transferred to a flat cell with diameter of 2.54
mm and path length of 1 mm immediately before the measurement. Within the cell,
yarns were positioned in a random orientation. SANS measurements were conducted at 5
h and 36 h following D2O immersion to monitor changes in the scattering profiles, which
will reflect the exchange of D2O and H2O in the pore spaces of the fiber.
After calibration and taking into account the sample transmission and thickness,
two-dimensional SANS images, shown in Figure 3(a), were averaged azimuthally to
produce a one-dimensional plot of the absolute scattered intensity as a function of the
scattering wave vector q (q= 4π sin(θ /2)/λ, where θ is the scattering angle and λ is the
wavelength). This plot is also referred to as the scattering profile. If the two-
dimensional scattering image exhibits a preferred orientation, a sector average was
10
accounted for over an azimuth angle of 15 degrees, as indicated in Figure 3(b). A peak in
the scattering profile or a ring in the scattering image at scattering wave vector q
indicates the existence of an ordered micro/nanodomains with a characteristic average
length d= 2π/q [6].
Atomic Force Microscopy—The nanoscale surface morphology of the fibers was
observed using atomic force microscopy (AFM), using a Dimension 3100 scanning probe
microscope (Veeco Metrology) in tapping mode. All scans were taken using commercial
silicon microcantilever probes (Veeco Metrology) with a manufacturer-reported radius of
< 10 nm. Topographic and phase images were obtained simultaneously using a
resonance frequency of approximately 300 kHz for the probe oscillation and a free-
oscillation amplitude of 62 nm ± 2 nm. Between 6 and 10 micrographs were obtained for
each sample, with representative images reported here.
Laser Scanning Confocal Microscopy—A Zeiss Model LSM510 reflection laser
scanning confocal microscope (LSCM) was used to characterize the surface morphology
of the fibers. The incident laser wavelength was 543 nm. By moving the focal plane in
the z-direction, a series of single images (optical slices) can be stacked and digitally
summed over the z-direction to obtain a 3-D image. All images presented here are 2-D
projections of a stack of 3-D images. The z-direction step size was 0.1 µm using a 150x
objective.
Sealed Tube Study—Approximately 200 specimens having a length of 51 cm
were cut from a spool of virgin PBO yarn supplied by the manufacturer. Each length of
yarn was inserted into a 6 mm diameter glass tube, which was then evacuated and back-
filled with argon, after which the tube ends were heat-fused. Tubes were then placed in a
11
55 oC circulating air oven and removed at periodic intervals for tensile testing and FTIR
analysis. A thermocouple sealed into one of the argon-purged tubes confirmed that the
temperature in the tube reached 55 oC after being placed in the oven. Between 10 and 13
specimens were randomly selected and tested at predetermined time intervals. Elapsed
time between removal of the yarn from the glass tube and either tensile testing or infrared
analysis was less than 5 min.
Results and Discussion
PBO is a member of the benzazole polymer family and is characterized by the
heterocyclic benzobisoxazole group in its main chain structure. The chemical structure
of the PBO repeat unit is shown in Figure 4. The conjugated benzobisoxazole and
phenyl rings in the PBO repeat unit contribute to extended π-electron delocalization and
molecular rigidity, which provides high thermal stability and outstanding mechanical
properties. PBO fibers, as are the majority of the polybenzazole-based fibers, are
extremely strong, tough and stiff, with tensile strengths and moduli greater than that of
polyaramid or ultra-high molecular weight polyethylene. The chemistry and processing
of PBO and related polymers have been documented elsewhere [7,8] and are not
discussed further.
Figure 5 shows the relative humidity sensor readings from the interior of the
environmental chamber as well as from the interior of the ballistic panel, during a period
when the relative humidity setting within the chamber was deliberately decreased and
then increased. The sensor inside the ballistic panel responded to these changes rapidly,
12
indicating that water vapor in the external environment is readily transmitted through
both the cotton carrier and the moisture-permeable liner into the ballistic panel. For this
particular model of body armor, moisture that is present in the external environment or on
the wearer’s body is readily transported into the ballistic fabric.
Moisture sorption measurements were carried out on virgin PBO spool yarn to
determine the mass uptake of water during the temperature/humidity exposure period. In
the desorption stage of the experiment, the moisture content of the virgin PBO yarn
stored under ambient conditions was approximately 0.8 mass % to 0.9 mass %, which
compares well with mass loss at 110 oC measured via thermogravimetric analysis (TGA).
As shown in Figure 6, the equilibrium moisture content of the virgin yarn at 50 oC and 60
% RH and 60 oC and 37 % RH is (1.56 ± 0.02) mass % and (0.81 ± 0.02) mass %,
respectively, with the higher temperature condition resulting in a lower mass uptake of
water. Lower moisture uptake at higher temperatures has also previously been observed
for poly(p-phenylene terephthalamide) (PPTA), another commonly used ballistic material
[9, 10], and nylon 6,6 [11].
Figure 6 also shows the sorption behavior of the PBO yarn at 50 oC and 60 % RH
followed by an in-situ change in the experimental conditions to 60 oC and 37 % RH. The
moisture content of the yarn decreases at the higher temperature, which is consistent with
previous observations, but does not completely reach the moisture content of the yarn
initially equilibrated at 60 oC and 37 % RH. One possible explanation for this difference
of 0.2 mass % between the two equilibrium moisture levels is that the microvoids in the
fiber trap adsorbed water, and this trapped water is not easily removed at the temperature
and relative humidity level used [12].
13
Figure 7 shows the moisture sorption isotherm for virgin spool yarn at 40 oC,
which is approximately the temperature of the human body under normal conditions. The
sorption isotherm provides information on the water sorption in PBO fibers as a function
of relative humidity at a given temperature. At high levels of relative humidity, the
moisture content of the PBO fibers approaches 7 mass % at 95 % RH. Analysis of the
sorption isotherm was carried out using the Guggenheim-Anderson-de Boer (GAB)
model, which has been shown suitable for describing water sorption isotherms of a
variety of polymers over a wide RH range [13]. The experimental water sorption
isotherm was fitted by the GAB equation, which has the form:
( ) ( ),
,11
1 1w
GAB P GAB w
w P GAB wa
m C kamka C ka
= ×− + −
(1)
where aw is the water activity (i.e. RH/100), maw is the water content at a specific value
of aw, Cp,GAB is the Guggenheim constant, mGAB is the monolayer water content and k is a
correction factor which is typically less than 1. To determine these parameters, the GAB
equation is linearized to the following expression:
( ),
, ,
111
w
p GABwGAB w
w a p GAB GAB p GAB GAB
Caf aka m C m k C m
−= = +
− (2)
A plot of GABf versus wa within the range 0.1< wa < 0.8 gives a linear plot if a correct
value of k is used, and whose intercept and slope are ,
1
p GAB GABC m kand ,
,
1p GAB
p GAB GAB
CC m
−
respectively. The GAB parameters obtained for the sorption isotherm at 40 oC for the
virgin yarn are shown in Figure 7. The residual sum of squares (RSS) values defined by
14
( )exp calcRSS m m= −∑ show a good fit between the experimental data and the model
over the entire range of relative humidity.
As shown in Figure 7, the moisture sorption isotherm of the PBO fibers at 40 oC
displays an upward curvature which became more pronounced at higher relative
humidity. The positive deviation from linearity, i.e. from Henry’s law, at high relative
humidity suggests that the clustering of water occurs in the fibers. The number of water
molecules in a cluster can be estimated from the GAB parameters and φ, the volume
fraction calculated as the ratio of the volume of sorbed water at the sorption equilibrium
to the volume of dry polymer. Values of φ were determined from the moisture content
using a fiber density of 1.54 g/cm3 [3]. The cluster number, Nc, represents the average of
excess water molecules in the vicinity of a given water molecule including itself, and can
be expressed as follows [14]:
( ), ,,
(1 ) 2 2 2 1C P GAB w w P GABGAB P GAB
N C ka ka Cm Cϕϕ
⎡ ⎤⎢ ⎥⎢ ⎥⎣ ⎦
= − − × − + + − − (3)
If Nc is equal to unity, then no clustering exists.
Figure 8 shows the number of water molecules per cluster in the PBO yarn as a
function of relative humidity at 40 oC. In the relative humidity range from 0 % to 20 %,
no clustering was observed. The number of water molecules increases in a near-linear
fashion in the relative humidity range between 20 % and 60 %, coinciding with the point
of inflection in the water sorption isotherm. In the range between 20 % and 60 %, Nc is
approximately 2. Beyond 60 % RH, Nc increases rapidly up to 8.3 water molecules per
clusters at 95 % RH. Cluster growth results when a higher affinity exists between water
molecules than between water molecules and the fiber, and is also attributed to the
15
presence of microcavities and micro-cracks, which increase the capacity for moisture
sorption.
The moisture sorption mechanism of PPTA, another commonly-used ballistic
fiber, has been studied extensively by other researchers [9, 12]; however, little or no data
on the moisture sorption behavior of PBO has been published until now. The chemical
composition and the microstructure of fiber materials are two parameters that strongly
influence water vapor sorption behavior. Kitagawa et al. proposed that the PBO fiber is
composed of microfibrils and that capillary-like microvoids are present between the
microfibrils [15]; a similar microstructure has also been attributed to PPTA [16,17,18].
In contrast to PPTA which contains amide and amino functional groups that are capable
of hydrogen-bonding with water, PBO has functional groups that are polar in nature but
not capable of hydrogen-bonding.
Table 1 shows tensile strengths of vest yarns subjected to environmental chamber
aging as a function of exposure time. The tensile strength of unaged vest yarns is 4.8
GPa, compared to the virgin PBO spool yarn tensile strength of 5.3 GPa measured in our
lab and 5.8 GPA reported by the manufacturer [3]. The difference between the tensile
strengths of the unaged vest yarn and the virgin yarn is attributed to mechanical damage
incurred in the weaving process.
At 50 °C and 60 % RH, average yarn tensile strength dropped from 4.8 GPa to
3.64 GPa after 84 d. The rate of tensile strength loss was determined not to be
statistically different for yarns extracted from the two vests and appears to be near-linear
with time. In an attempt to accelerate the rate of degradation, the chamber temperature
was increased to 60 °C while maintaining the chamber moisture content at the same level
16
by decreasing the relative humidity to 37 %. Exposure continued for another 73 d, during
which the average yarn tensile strength dropped from 3.64 GPa to 3.08 GPa. No
additional decreases in tensile strength were observed during storage at 25 oC and 5 %
RH. Average strain to failure during the exposure period dropped from 3.31 % to 2.17 %
while the tensile modulus remained constant at around 145 GPa.
Tensile strengths of single fibers measured via DMTA are compared with yarn
tensile strength data in Figure 9. In general, the fiber data track closely with and come
close to overlapping the yarn data, when the data standard deviations are taken into
account (which are greater for the single fiber than they are for the yarn). The advantage
of testing single fibers as opposed to yarns is the amount of material needed for the
respective tests: DMTA can be used to test fibers as short as 12 mm, whereas a full 51
cm is needed for a yarn tensile test on a typical universal test frame.
The interaction between materials and the infrared region of the electromagnetic
spectrum provides valuable information on the molecular structure of organic materials,
including organic polymers. Specific functional groups absorb at given frequencies
corresponding to their vibrational modes. Changes in the intensities or frequencies of
observed spectral peaks can be used to elucidate changes in the molecular structure of the
compound. This type of information is valuable for mechanistic and kinetic studies of
polymer degradation. The primary infrared bands in PBO are listed and assigned in
Table 2. Peak identification and assignments are made on the basis of literature data [19,
20, 21, 22, 23] and studies carried out in our lab on benzoxazole and 2-phenyl
benzoxazole model compounds.
17
ATR-FTIR analysis of extracted vest yarns was carried out concurrently with
tensile testing. Figure 10 shows the ATR infrared spectra of the yarns prior to and after
environmental aging for 157 d. Visual examination of the two spectra, which have been
baseline-corrected and normalized, shows distinct peak intensity differences.
These differences are most easily analyzed using spectral subtraction, in which a
reference spectrum is subtracted from the spectrum of a material of interest. This
technique is often helpful in extracting specific chemical changes and providing
information on the formation and depletion of specific functional groups. Figure 11
shows the difference spectra that result when the infrared spectrum of the non-exposed
vest yarn is subtracted from each of the exposed vest yarn spectra. Downward-pointing,
or negative, peaks in the difference spectra are attributed to species that are lower in
concentration relative to the reference spectrum (the non-exposed vest yarn) and upward-
pointing, or positive, peaks are either species that are higher in concentration relative to
the reference material or are new species that were not originally present in the reference
material.
Negative peaks observed at 914 cm-1, 1056 cm-1, and 1362 cm-1 are assigned to
the vibrations associated with the benzoxazole ring [19], and grow progressively larger
(more negative) with time. A positive peak at 1650 cm-1 in the region associated with
amide carbonyl or carboxylic acid [24] also grew progressively larger with time. This
observation suggests that benzoxazole ring-opening has occurred with the subsequent
formation of benzamidophenol groups as depicted in Figure 12. Further breakdown of
benzamidophenol groups could lead to the formation of aminophenol and benzoic acid
groups, and the breadth of the peak at 1650 cm-1 allows for the possibility of benzoic acid
18
peak at 1680 cm-1 [24]. The growth of new peaks centered at 3300 cm-1 also points to
the presence of amide N-H stretch or carboxylic acid O-H stretch.
Kim et al. [25] observed carboxylic acid peaks in the FTIR spectra of PBO that
have undergone acid-catalyzed hydrolysis, with a concurrent decrease in the molecular
weight evidenced by significant decrease in intrinsic viscosity, which is consistent with
the chain scission mechanism. Evidence for PBO hydrolysis leading to carboxylic acid
formation is also reported by So et al., who detected a peak at 1690 cm-1 attributed to
carboxylic acid in the infrared spectrum of PBO, following exposure to severe hydrolytic
conditions [26].
Support for the hydrolysis of benzoxazole to benzamide in low molecular weight
compounds was given by Jackson et al [27]. When 2-phenylbenzoxazole (1) is heated in
an acidic medium, N-(2-phenylhydroxybenzamide) (2) is first formed:
(1) (2)
N-(2-phenylhydroxybenzamide) can then further hydrolyze to 2-aminophenol and
benzoic acid ((3) and (4), respectively), or re-convert to 2-phenylbenzoxazole (1):
(2) (3) (4)
N
O
N
O
NH-C-
OH
O
NH-C-
OH
O
NH-C-
OH
O
NH-C-
OH
ONH2
OH
NH2
OH
COOHCOOH
19
Two small peaks are observed at 1726 cm-1 and 1691 cm-1 in all yarns analyzed,
and are shown on an expanded scale in Figure 13. These peaks have not been reported in
any previous publications on PBO and have not been observed in our analysis of
benzoxazole-containing model compounds. However, FTIR analysis of phenyl benzoate
compounds revealed a match to these 2 peaks. 2-phenyl benzoate is an intermediate
compound in the synthesis of PBO, which undergoes acyl migration to form the
corresponding 2-phenylhydroxybenzamide, which then subsequently rearranges to form
the benzoxazole ring structure [28]. It is possible that the phenyl benzoate peaks detected
in the FTIR spectrum of PBO are due to residual intermediate products from the synthesis
process. The presence of these residues is potentially detrimental to PBO properties,
because benzoate linkages are not as chemically, hydrolytically, or thermally resistant as
benzoxazole linkages, and each benzoate linkage exists at the expense of the more
desirable benzoxazole functionality.
Figure 14 shows yarn tensile strength plotted against the absorbance of the
negative peaks corresponding to the benzoxazole group. A positive correlation was
observed between tensile strength and spectral absorbance of these peaks; that is, as the
benzoxazaole group decreases in concentration due to hydrolysis, the tensile strength of
the yarns decreases. Benzoxazole hydrolysis causes tensile strength degradation in PBO
by disrupting the conjugated rigid rod structure and replacing it with a polyaramid-type
structure. Subsequent hydrolysis of the benzamide group causes chain scission and
molecular mass decrease, which also contributes to tensile strength degradation [29].
Additional evidence for the breakdown of PBO structure is provided by the SANS
analysis. Figure 15 compares SANS images of (a) virgin PBO in D2O for 5 h, (b) virgin
20
PBO in D2O for 36 h, (c) unaged vest yarn in D2O for 5 h, and (d) vest yarn aged for 157
d in the environmental chamber, in D2O for 5 h. For unaged and aged vest yarns, the 2D
SANS images for 5 h and 36 h were indistinguishable. The corresponding vertical-sector
averaged scattered intensity of these three yarns as a function of wavevector, q, are
plotted in Figure 16 at 5 h and 36 h.
As shown in Figure 15(a), the 2D SANS image of virgin PBO displays a
diamond-shaped scattering pattern, which is indicative of an ordered nanostructure
aligned along both the vertical and horizontal directions. After 36 h in D2O, the relative
scattered intensity of the virgin PBO fiber, as shown in Figure 15(b), decreased
noticeably, although the diamond shape of the scattering pattern remains the same. This
intensity change is believed to reflect the exchange of D2O and H2O in the pore spaces of
the fiber, which reduces the contrast of scattering between the nanodomain and its
surroundings. The lack of changes in the shape of the scattering pattern indicates that no
changes in the nanostructure of the fiber have occurred between 5 h and 36 h. The
vertical sector averaged scattered intensity for the virgin PBO at 5 h and 36 h, shown in
Figure 16, also shows a noticeable difference in intensity near q ≈ 0.3 nm-1. A broad
peak (noted as Point A) is observed in the scattering profile of virgin PBO, and the
corresponding length scale of the features that gave rise to this peak is estimated to be
approximately 20 nm.
It was expected that the nanostructure of the unaged vest yarn would be similar to
that of the virgin PBO; however, the SANS image of the unaged vest yarn (Figure 15(c))
exhibits a vertically preferred pattern only. This result indicates that the ordered-
nanodomains were aligned along the horizontal with respect to the incident neutron
21
direction. No changes in the scattering patterns or scattering profiles were observed
between the 5 h and 36 h measurements, in contrast to the behavior of the virgin PBO
yarn. It is speculated that D2O diffusion into the vest yarns occurred completely in the
first 5 h, and that no additional diffusion of D2O occurred between 5 and 36 h. This
phenomenaon could be due to differences in internal nanostructure between the virgin
PBO spool yarns and the yarns extracted from woven vest fabric, or the fact that there are
more damage sites in the vest yarns that provide additional pathways for D2O ingress. A
broad peak at point B in Figure 16, originating from features with length scale
approximately 15 nm, is observed in the 15o vertical sector averaged intensity for the
unaged vest yarn.
Unlike the SANS images of virgin PBO and unaged vest yarn, the SANS
scattering pattern of an aged vest yarn, shown in Figure 15(d), appears to be symmetrical.
There is no peak observed in the scattering profiles shown in Figure 16. This scattering
profile is similar to that from a random multi-scale structure polymer solution and no
ordered nanostructure dominates; i.e. it is postulated that the ordered-nanodomains
observed in both the virgin and unaged PBO yarns have broken down after 157 d of
environmental exposure. SANS has provided information on PBO nanostructure that is
not provided by any other technique. Detailed interpretation of the results, however, will
require more controlled experiments to be performed in the near future.
Laser scanning confocal microscope (LSCM) was used to image fibers taken from
the vests prior to exposure and after 157 d of exposure, as shown in Figure 17. The
vertical banding shown in both micrographs is attributed to mechanical damage incurred
22
during the weaving process. At the level of observation, no significant changes in surface
morphology were observed in the yarns aged for 157 d relative to the unaged yarn.
Atomic force microscopy (AFM) was employed to examine the fiber surface on a
smaller scale. Figure 18(a) shows AFM micrographs of the surface of a virgin fiber
compared with the surface of a fiber extracted from a woven vest in Figure 18(b). The
fiber after weaving, as shown in Figure 18(b), is considerably rougher than the virgin
fiber shown in Figure 18(a), further supporting the speculation that mechanical damage is
incurred during weaving. This speculation is further reinforced by the comparison of the
root mean square roughness (Rq) values of approximately 4 nm for the virgin fiber and
approximately 10 nm for the fiber extracted from the woven fabric.
AFM micrographs of fiber surfaces as a function of elevated temperature and
humidity exposure are shown in Figure 19. As exposure time increases, this surface
roughness also increases. After 9 weeks of exposure (Figure 19(b)) the surface roughness
has increased from an Rq of approximately 10 nm to an Rq of approximately 13 nm,
however the underlying smooth surface structure is still visible in some areas. After 14
weeks of exposure (Figure 19(c)) the fiber is somewhat smoother, with an Rq value of 6
nm. This lower Rq could be attributed to a sloughing off of some of the larger rough
areas of the fiber, thereby exposing the smoother surface underneath. The micrograph
taken at 22 weeks (Figure 19(d)) shows a very rough surface, with an Rq value of
approximately 20 nm. All traces of the smooth underlying structure seen in Figure 19(a)
are completely gone, indicating major degradation of the surface of the fiber.
Tensile testing of the yarns sealed in argon-purged tubes was carried out to
determine if the small amount of residual moisture in the fiber was sufficient to initiate
23
chemical and mechanical degradation. Strength retention data in Figure 20 shows that
the sealed tube yarns exhibited less than 4 % loss in tensile strength over the 210 d
exposure period, compared to 40 % tensile strength degradation in the same period of
time for the yarns exposed to elevated temperature/relative humidity. This result, along
with the tensile strength data of yarns extracted from vests placed in a 25 oC and 5 % RH
environment, suggest that moisture is an operative factor in chemical hydrolysis, leading
to the loss of PBO tensile strength.
The absence of oxygen in the sealed tubes raised the question of whether oxygen
alone in or in synergy with moisture could be implicated in PBO degradation. Thermo-
oxidative aging studies carried out by researchers at Sandia National Laboratories on
nylon 6,6 indicated that the presence of oxygen accelerated hydrolytic degradation
mechanisms [30]. It was not feasible to repeat the sealed tube experiments with an
oxygen or air atmosphere; however, in isothermal thermogravimetric experiments
carried out on PBO yarns in air at 50 oC, mass loss was less than 1 mass % after 18 h.
This result suggests that oxidative degradation is not an expected degradation pathway at
the temperature employed in the study.
Infrared difference spectra for the yarns aged in the sealed tubes, referenced to
virgin PBO, are shown in Figure 21. The largest peak magnitudes are observed for yarns
aged for 4 weeks, after which all peaks (positive and negative) grow progressively
smaller. The difference spectrum for the 20 week yarn approaches a flat line, indicating
that it is almost identical to the virgin PBO reference spectrum. It is postulated that the
process of sealing the fibers into the tubes created a reversible perturbation into the
system, which gradually dissipated as the aging study commenced. The peak changes
24
observed in the elevated temperature/humidity study are not in evidence here, and no sign
of benzoxazole hydrolysis is observed.
Summary and Conclusions
Tensile strength of yarns extracted from ballistic panels aged at elevated
temperature and relative humidity exhibited approximately 40 % loss in strength over a
157 d period. FTIR analysis of yarns exposed to elevated temperature/relative humidity
indicated benzoxazole ring opening to yield amide functionality, and subsequent
hydrolysis of amide to carboxylic acid and aminophenol groups. Analysis of the fiber
surface morphology indicated a surface roughening as a function of exposure time.
SANS analysis also revealed differences between the internal structure of virgin PBO
spool yarn as compared to PBO vest yarns, in that diffusion of D2O in the pore spaces of
virgin PBO occurred at a slower rate. The scattering profiles of virgin yarn and unaged
vest yarn showed internal structure corresponding to size scales between 15 nm and 20
nm, whereas the vest yarns that had undergone 157 d of aging showed no organized
nano-structural features in the 20 nm to 200 nm range.
When external moisture was decreased to very low levels, either via storage in a
25 oC and 5 % RH environment or in argon-purged sealed tubes, changes in yarn tensile
strength were less than 4 % and no benzoxazole ring opening was observed via FTIR.
These results indicate that one of the main degradation mechanisms in PBO fiber is
initiated by moisture, but that moisture inherent in the fiber is not the primary initiator of
degradation.
25
Acknowledgements
The authors gratefully acknowledge project funding provided by the National Institute of
Justice (NIJ) as well as the assistance of Ron Rise and Steve Lightsey of the Tekne Group in
tensile testing, Nathaniel Waters of NIST’s Office of Law Enforcement Standards (OLES) in
setting up the temperature/humidity chamber exposures, and Jeff Anderson of the Fabrication
Technology Division for preparing the sealed tube samples.
26
Table 1: Tensile properties of vest yarns during environmental chamber exposure (50 °C/60% RH, 0 days to 84 days, followed by 60 °C/37% RH , 85 days to 152 days); values are averages from all layers tested in two vests. Relative standard uncertainties are typically ± 3 % for tensile strength, ± 3 % for strain, ± 3 % for modulus, and ± 4 % for break energy.
Time in Chamber
Tensile Strength
Strain at Break Modulus Energy to
Break Point (d) (GPa) (%) (GPa) (N m) 0 4.82 3.31 141.06 0.76
15 4.45 3.09 142.48 0.65
29 4.18 2.96 142.68 0.58
44 4.02 2.88 141.60 0.54
56 3.88 2.73 147.11 0.50
71 3.80 2.71 144.59 0.49
85 3.64 2.55 147.97 0.44
98 3.50 2.50 145.78 0.42
109 3.57 2.51 146.66 0.43
118 3.51 2.48 146.53 0.42
132 3.30 2.40 147.76 0.39
146 3.23 2.28 147.39 0.35
152 3.30 2.31 148.92 0.37
157 3.08 2.17 146.99 0.32
27
Table 2: FTIR-ATR Band Assignments for PBO Fiber
Band Assignment (cm-1) 3097 Aromatic C-H stretch from benzene between oxazole rings, closer to oxygen 3069 Aromatic C-H stretch from benzene between oxazole rings 3040 Aromatic C-H stretch from phenyl ring 2956 Aliphatic C-H stretch (sizing) 2910 Aliphatic C-H stretch (sizing) 2851 Aliphatic C-H stretch (sizing) 1726 1691 1619 C=C stretching in substituted aromatic rings, cyclic C=N stretching 1577 Skeletal vibrations in conjugated system/benzoxazole ring 1557 Skeletal vibrations in conjugated system/benzoxazole ring 1496 Skeletal vibrations in conjugated system/benzoxazole ring 1461 Skeletal vibrations in conjugated system/benzoxazole ring 1412 1367 1329 C-N stretching 1308 C-N stretching 1276 C-C stretching in carbons linking oxazole and aromatic ring; O-C=N stretching 1210 1147 Asymmetric stretching of unsaturated cyclic ether 1114 Aromatic C-H in-plane bending 1056 Asymmetric stretching of unsaturated cyclic ether 1010 Aromatic C-H in-plane bending 925 Symmetric C-O-C stretching of cyclic ether 914 Symmetric C-O-C stretching of cyclic ether 869 Aromatic C-H out of plane bending 848 Aromatic C-H out of plane bending 821 Aromatic C-H out of plane bending
30
(a)
(b)
Figure 3: Two-dimensional SANS images of (a) isotropic, and (b) preferred orientation scattering profiles. In (b) a vertical sector average region of 15 degrees is also illustrated.
31
CC
CC
CC
CC C
C C
C
CC
N N
O OH H
H HH
H
CC
CC
CC
CC C
C C
C
CC
N N
O OH H
H HH
H
CC
CC
CC
CC C
C C
C
CC
N N
O OH H
H HH
H
CC
CC
CC
CC C
C C
C
CC
N N
O OH H
H HH
H
Figure 4: Chemical structure of poly(p-phenylene-2,6-benzobisoxazole), or PBO.
n
32
y
2/20
4:0
0
2/20
8:0
0
2/20
12:
00
2/20
16:
00
2/20
20:
00
Hum
idity
, %R
H
0
10
20
30
40
50
60
Top Shelf, FrontTop Shelf, BackMiddle Shelf, FrontMiddle Shelf, BackInside Vest
Figure 5: Relative humidity sensor data from environmental chamber, comparing relative humidity at various locations in the chamber to the internal relative humidity of the vest. In the time interval between the dashed lines, the relative humidity settings on the environmental chamber were deliberately decreased and then increased. The estimated uncertainty of the data is ± 2 % RH.
33
Figure 6: Moisture uptake for virgin PBO yarn measured in separate experiments at (a) 50 oC and 60 % RH, (b) 60 oC and 37 % RH, and (c) 50 oC and 60 % RH and 60 oC and 37 % RH followed by 60 oC and 37 %RH. The estimated uncertainty of the data is ± 0.02 mass %.
0.0
0.2
0.4
0.6
0.8
1.0
1.2
1.4
1.6
1.8
0 500 1000 1500 2000 2500Time (min)
Moi
stur
e C
onte
nt (m
ass
%)
0 100 200 300 400 500 600 700 800 900 1000
50 C/60 % RH followed by 60 C/37 % RH
50 C/60%RH
60 C/37 %RH
34
0
1
2
3
4
5
6
7
0 10 20 30 40 50 60 70 80 90 100
Relative humidity (%)
Moi
stur
e C
onte
nt (
mas
s %
)
Experimental dataGAB model
Cp,GAB mGAB (%) k RSS
2.498 1.00 0.90 0.00977
Figure 7: Water sorption isotherm of virgin PBO yarn at 40 oC. The table provides the parameters obtained from fitting the sorption data to the GAB model.
35
0
1
2
3
4
5
6
7
8
9
0 10 20 30 40 50 60 70 80 90 100Relative humidity (% )
Nc
Figure 8: Number of water molecules per cluster, Nc, in virgin PBO yarn, as a function of relative humidity at 40 oC.
36
0
1
2
3
4
5
6
7
0 25 50 75 100 125 150 175
Exposure Time (d)
Tens
ile S
treng
th (G
Pa)
YarnSingle Fiber
Figure 9: Tensile strength of single PBO fibers measured with DMTA compared to tensile strength of yarns measured on a test frame. Error bars represent one standard uncertainty.
37
-0.1
0.1
0.3
0.5
0.7
0.9
1.1
80012001600200024002800320036004000
Wavenumber (cm-1)
Abs
orba
nce
0 days157 days
(a)
-0.1
0.1
0.3
0.5
0.7
0.9
1.1
800100012001400160018002000
Wavenumber (cm-1)
Abs
orba
nce
0 days157 days
(b)
Figure 10: FTIR spectra of PBO yarns extracted prior to and at the end of temperature and humidity aging. The relative estimated uncertainty of the data is ± 1 %.
38
-0.5
-0.4
-0.3
-0.2
-0.1
0.0
0.1
0.2
0.3
0.4
0.5
800130018002300280033003800
Wavenumber (cm-1 )
Abs
orba
ncec
e15 d29 d44 d56 d71 d85 d98 d109 d118 d132 d146 d157 d
-0.5
-0.4
-0.3
-0.2
-0.1
0.0
0.1
0.2
0.3
0.4
0.5
800100012001400160018002000
Wavenumber (cm-1 )
Abs
orba
nce
15 d29 d44 d56 d71 d85 d98 d109 d118 d132 d146 d157 d
Figure 11: Difference spectra for PBO yarns extracted from aged vests, referenced to spectrum of yarn taken at beginning of exposure.
39
N
O
N
O
NH-C-
OH
ON
O
HOOC-NH2
OH
N
O
N
O
N
O
N
O
N
O
NH-C-
OH
ON
O
NH-C-
OH
ON
O
HOOC-NH2
OH
N
O
HOOC-HOOC-NH2
OH
N
O Figure 12: Proposed degradation mechanism, showing benzoxazole (a) conversion to benzamidophenol (b), followed by hydrolysis to aminophenol (c) and benzoic acid (d).
(a)
(b)
(c) (d)
40
1.5E-02
2.0E-02
2.5E-02
3.0E-02
3.5E-02
4.0E-02
4.5E-02
160017001800
Wavenumber (cm-1)
Abs
orba
nce
Figure 13: Peaks at 1691 cm-1 and 1726 cm-1, observed in the infrared spectrum of all PBO yarns analyzed, tentatively attributed to the presence of phenyl benzoate.
16911726
41
2.50
3.00
3.50
4.00
4.50
5.00
0.00 0.05 0.10 0.15 0.20 0.25 0.30 0.35
Change in IR Peak Absorbance (absolute )
Tens
ile S
tren
gth
(MPa
)
914
1056
1362
1657
Figure 14: Tensile strength of PBO yarns from aged vests plotted versus the changes observed in infrared peak absorbance.
42
Figure 15: Two-dimensional (2D) SANS images of (a) virgin PBO yarn in D2O for 5 h, (b) virgin PBO yarn in D2O for 36 h, (c) unaged vest yarn in D2O for 5 h, and (d) vest yarn after 157 days of environmental chamber exposure, in D2O for 5 h. For unaged and aged vest yarns, the 2D SANS images for 5 h and 36 h were indistinguishable.
(a) (b)
(c) (d)
43
0.1 1
0.1
1
10
100
B, 15 nm
A, 20 nm
q(nm-1)
Virgin PBO, 5 h Virgin PBO, 36 h Unaged Vest Yarn, 5 h Unaged Vest Yarn, 36 h Aged Vest Yarn, 5 h Aged Vest Yarn, 36 h
Scat
tere
d In
tens
ity (a
.u.)
Figure 16: The 15o vertical sector averaged scattered intensity obtained from Figure 15 as a function of wavevector q, for three different yarns in D2O, measured at 5 h and 36 h. The estimated uncertainty of the data is 1 %.
44
(a)
(b)
Figure 17: Confocal images of (a) unaged PBO fiber from ballistic panel, and (b) PBO fiber following 157 d of exposure in environmental chamber.
45
(a)
(b)
Figure 18: AFM topographic images and corresponding surface Rq values for (a) surface of virgin PBO yarn, and (b) surface of PBO yarn extracted from unaged woven vest panel. All images are of a 3 µm x 3 µm area and the z scale for all images is 200 nm. The estimated uncertainty of the Rq values is ± 8 %.
Rq = 4 nm
Rq = 10 nm
46
(a) (b)
(c) (d)
Figure 19: AFM topographic images and corresponding surface Rq values for fibers extracted from ballistic panels following environmental chamber exposure at (a) 0 d, (b) 56 d, (c) 98 d, and (d) 157 d. All images are of a 3 µm x 3 µm area and the z scale for all images is 200 nm. The estimated uncertainty of the Rq values is ± 8 %.
Rq = 10 nm Rq = 13 nm
Rq = 6 nm Rq = 20 nm
47
0
20
40
60
80
100
120
0 50 100 150 200 250 300 350 400 450 500Exposure Time (d)
Stre
ngth
Ret
entio
n (%
)
Humidity Chamber, 50 C/60 % RH
Humidity Chamber, 60 C/37% RH
Humidity Chamber, 25 C/5 % RH
Sealed Tube, 55 C
Figure 20: Tensile strength of PBO yarns aged in sealed tubes, compared to tensile strengths of yarns extracted from vests aged in environmental chamber at 50 oC and 60 % RH followed by 60 oC and 37 % RH. Error bars represent one standard uncertainty.
48
-0.10
-0.05
0.00
0.05
0.10
0.15
0.20
0.25
800120016002000Wavenumber (cm-1)
Abs
orba
nce
4 weeks
6 weeks
10 weeks
14 weeks
18 weeks
22 weeks
30 weeks
Figure 21: Difference spectra for PBO yarns aged in sealed tubes, referenced to spectrum of virgin yarn.
49
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